Consider a simple circuit shown in figure stands for a variable resistance $R^{\prime} \cdot R^{\prime}$ can vary from $R_0$ to infinity. $r$ is internal resistance of the battery $(r<< R< R$,$) .$
Temperature dependence of resistivity $\rho(T)$ of semiconductors, insulators and metals is significantly based on the following factors
The measurement of an unknown resistance $R$ is to be carried out using Wheatstones bridge as given in the figure below. Two students perform an experiment in two ways. The first students takes $R_2=10 \Omega$ and $R_1=5 \Omega$. The other student takes $R_2=1000 \Omega$ and $R_1=500 \Omega$. In the standard arm, both take $R_3=5 \Omega$. Both find $R=\frac{R_2}{R_1}, R_3=10 \Omega$ within errors.
In a meter bridge, the point $D$ is a neutral point (figure).
Is the motion of a charge across junction momentum conserving? Why or why not?
When an electron approaches a junction, in addition to the uniform electric field $\mathbf{E}$ facing it normally. It keep the drift velocity fixed as drift velocity depend on $E$ by the relation drift velocity
$$v_d=\frac{e E \tau}{m}$$
This result into accumulation of charges on the surface of wires at the junction. These produce additional electric field. These fields change the direction of momentum. Thus, the motion of a charge across junction is not momentum conserving.